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REVIEW 3 major objections 5 minor 30 references

Investigating Lagrangian Neural Networks for Infinite Horizon Planning in Quadrupedal Locomotion

T0 review · 3 major / 5 minor · reviewed 2026-08-06 · deepseek-v4-flash

Pith's one-line read Lagrangian neural networks for quadruped dynamics beat generic neural networks in sample efficiency and prediction accuracy.

desk verdict A useful LNN-variant ablation on a quadruped, but the headline numbers and the diagonalization speed-up claim are not backed by the evidence; worth a round of revision, not a rejection. read the letter →

arxiv 2506.16079 v1 pith:KCUMCG4Q submitted 2025-06-19 cs.RO cs.LG

classification cs.ROcs.LG
keywords Lagrangianneuralnetworksquadrupedallocomotioninfinite-horizonplanningsampleefficiencymassmatrixdiagonalizationinversedynamicstrainingreinforcementlearningmodelpredictivecontrol
verification ladder T0 review T1 audit T2 compute T3 formal

The pith

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The reading

This paper argues that injecting Lagrangian physics structure into a learned dynamics model pays off in an infinite-horizon planning loop for a quadruped robot. It compares a generic multi-layer perceptron with four Lagrangian neural network variants: full forward-dynamics learning, a diagonalized mass-matrix version, inverse-dynamics training with forward inference, and a reduced torso-center-of-mass model. The reported results are that the LNN variants need roughly 10x fewer samples to learn the dynamics and predict future states 2-10x more accurately, with up to 85% lower prediction error on average than the baseline. The authors also claim the diagonalized formulation lowers the computational cost of forward dynamics enough to enable real-time receding horizon control. If these numbers hold, physics-structured models are a practical replacement for structure-agnostic networks inside model-based locomotion planners.

What carries the argument

The load-bearing object is the learned positive-definite mass matrix $M(q)=Y(q)Y(q)^T+\epsilon I$, where $Y(q)$ is a learnable lower-triangular matrix and $\epsilon I$ guarantees positive definiteness. Instead of learning the next state directly, the network builds a Lagrangian $L(q,\dot{q})=\dot{q}^T M_\theta(q)\dot{q}-V_\theta(q)$, and forward dynamics is obtained by inverting the Hessian in the acceleration equation. The paper's efficiency claim is carried by diagonalizing $M(q)=P(q)^T\Lambda(q)P(q)$ and rewriting the acceleration solve as $\ddot{q}=P(q)\Lambda(q)^{-1}P(q)^T(-C(q,\dot{q})\dot{q}-G(q)+Bu+F_{\text{ext}})$, so that the inverse reduces to a diagonal operation. Additional machinery includes inverse-dynamics training, which learns torques from accelerations and switches to forward inference at deployment, and a reduced-order center-of-mass state that shrinks the mass matrix.

What would settle it

Run the learned forward-dynamics model on the real 18x18 mass matrix in the paper's setup and time the diagonalized acceleration equation against direct inversion or Cholesky factorization; if inversion is not slower, the diagonalization speed-up and real-time control claim fails.

Watch

Extended reading notes

Core claim

The central discovery is that a Lagrangian Neural Network that learns the mass-inertia matrix $M(q)=Y(q)Y(q)^T+\epsilon I$, rather than directly regressing future states, captures quadruped dynamics more efficiently and accurately than an MLP baseline within the paper's dreaming and planning loop. Across the four studied variants, the structured models show faster loss reduction per iteration, better forward prediction accuracy, and a 10x sample-efficiency improvement; the forward LNN attains the lowest prediction error, with inverse-dynamics-trained LNN close behind, and the diagonalized mass-matrix version provides the computational path to real-time receding horizon control while preserving physical interpretability.

Load-bearing premise

The real-time speed claim assumes that eigendecomposing the learned mass matrix at inference is cheaper than directly inverting or factorizing it, an assumption the paper states but does not measure.

Editorial extensions

If this is right

  • An LNN-based dynamics model can replace the structure-agnostic MLP inside the planning loop and produce lower prediction error over long horizons.
  • The diagonalized mass-matrix formulation makes forward-dynamics inference cheap enough to run inside a receding horizon controller on a quadruped.
  • Training an LNN with inverse dynamics is a viable shortcut: it avoids some numerical issues of matrix inversion while keeping prediction accuracy close to the forward-LNN model.
  • The torso-center-of-mass reduced LNN trades accuracy for speed and still behaves competitively with the baseline MLP.
  • The observed 10x sample-efficiency improvement means less simulator data is needed to learn a usable quadruped dynamics model.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • The real-time speed claim actually depends on an unmeasured comparison: eigendecomposing the learned mass matrix at inference must be cheaper than inverting or factorizing it, and a wall-clock benchmark on the 18x18 matrix would decide this.
  • Because inverse-dynamics training avoids the acceleration solve during learning, an obvious extension is to have the policy output accelerations or torques directly, which would remove the actuator-network conversion the authors flag as a bottleneck.
  • Numerical eigendecomposition is not exact; a closed-loop test comparing the diagonalized acceleration equation against direct inversion would reveal whether eigenvector error degrades long-horizon predictions.
  • The CoM-reduced LNN's error being close to the generic baseline suggests a hybrid planner could use the cheap CoM model for most of the horizon and the full-order LNN only at safety-critical steps.
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Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, and a circularity audit.

Referee Report

3 major / 5 minor

Summary. The paper presents an empirical study of four Lagrangian Neural Network (LNN) variants--full-order forward dynamics, diagonalized mass-matrix forward dynamics, inverse-dynamics training with forward-dynamics inference, and a reduced-order center-of-mass model--as learned dynamics models inside the PIP-Loco infinite-horizon planning framework for a simulated Unitree Go1 quadruped. The central claims are that physics-structured LNN dynamics are more sample-efficient (10x) and more accurate (up to 2-10x) than a structure-agnostic MLP baseline, and that diagonalizing the learned mass matrix reduces computational complexity, enabling real-time receding horizon control. The experiments reported are dynamics-loss curves, prediction-error curves, and controller inference-frequency box plots; no closed-loop planning results or wall-clock comparisons are provided.

Significance. If properly supported, the empirical comparison of LNN variants against an MLP baseline for quadruped dynamics would be a useful ablation, confirming that physics-inspired parameterizations can improve sample efficiency and prediction accuracy in a high-dimensional legged system. The paper also clearly identifies four distinct modeling choices that practitioners could adopt. However, the computational-efficiency claim is central to the abstract and is currently unsupported; the paper also does not evaluate the learned dynamics inside the actual planning loop or report closed-loop task performance. The contribution is therefore promising but not yet established at the level claimed.

major comments (3)
  1. [III.A, Eqs. (10)-(14)] The claimed computational speed-up from diagonalizing the mass matrix is not established and is likely incorrect as stated. Because M(q) = Y(q)Y(q)^T + epsilon*I is a learned matrix-valued function, the matrices P(q) and Lambda(q) must be obtained by a full symmetric eigendecomposition at every inference step, which is an O(n^3) operation with a larger constant than directly solving Eq. (8) via Cholesky factorization or a general linear solve. The statement that Lambda being diagonal makes its inverse cheap is mathematically true but does not reduce the dominant cost of computing the eigendecomposition. The paper provides no wall-clock comparison between Eq. (14) and direct inversion, and Figure 5 reports controller frequency, not the per-step cost of the dynamics prediction. Furthermore, Figure 4 omits the 'LNN Diagonalised' model entirely, so there is no evidence that the diagonalized variant preserves the prediction accuracy of the forward LNN. Since the abstract's 'real-time receding horizon control' claim rests on this computational argument, the authors must either provide a proper timing benchmark or remove the claim.
  2. [IV, Figures 3-4] The headline quantitative claims--10x sample efficiency, up to 2-10x prediction accuracy, and an average 85% reduction in prediction error--are not supported by any numerical data in the text. Figure 3 plots normalized loss on a logarithmic scale, but 'sample efficiency' is never defined operationally, no threshold crossing is reported, and no iteration counts are given. Figure 4 shows prediction-error curves without axis values, final errors, or per-model numbers, and the 'up to 85%' figure is not tied to a specific method or time step. Because these numbers appear in the abstract as experimental results, they should be backed by a table or explicit statistics, preferably with multiple seeds and error bars.
  3. [IV, Deployment Scheme] The paper does not evaluate the proposed dynamics models inside the infinite-horizon planning loop described by Eqs. (17)-(18). The experiments measure only dynamics prediction error and controller frequency, not closed-loop task performance such as tracking error, reward, or success rate in the PIP-Loco framework. The abstract's claims about 'infinite horizon planning' and 'real-time receding horizon control' therefore go beyond the evidence presented. A closed-loop comparison of LNN-based and BNN-based planning, or a clear repositioning of the paper as a dynamics-model-only study, is needed.
minor comments (5)
  1. [Abstract] The abstract states '10x' and '2-10x' without the qualifier 'up to,' which is inconsistent with the later 'up to 85%' phrasing; these claims should be precisely quantified or qualified.
  2. [IV, Inference Speed Analysis] The text says that physics-inspired approaches 'tend to have lower inference frequencies,' which appears in tension with the abstract's claim of a higher control frequency than previous LNN methods; please clarify which specific prior method is being compared and report the numerical frequencies.
  3. [Figure 5] The y-axis label 'Frequency' lacks units; please specify Hz or control-loop iterations per second, and describe what the 'candle plots' represent.
  4. [III.A, Eq. (15)] The inverse-dynamics training objective is trained with Eq. (15) but deployed with forward dynamics Eq. (8); the paper should comment on whether this train/inference mismatch affects stability, since the inverse-trained model never directly minimizes forward-dynamics prediction error.
  5. [IV, Results] There are several typographical and clarity issues: 'sample efficieny' should be 'sample efficiency,' the term 'candle plots' should be clarified, and Figure 3's normalization procedure should be defined in the caption or text.

Circularity Check

0 steps flagged · score 2.0 of 10

No significant circularity: the LNN-vs-BNN gains rest on independent baselines, and the diagonalization concern is an unsupported efficiency claim rather than a circular reduction.

full rationale

The paper's central quantitative claims—10x sample efficiency and up to 85% (2-10x) prediction-error improvement—are empirical comparisons between LNN variants and a structure-agnostic MLP (BNN) trained and evaluated on the same data. These numbers are not constructed from the LNN definition, and the BNN is an independent baseline, so the main comparison is not circular. Equations (6)-(8) are standard LNN constructions from prior external work [11], not self-referential definitions. The diagonalization step (Eqs. 10-14) is a mathematically valid spectral decomposition: Eq. 14 is algebraically equivalent to Eq. 8, and the paper's assertion that it 'reduces computational complexity and enables faster inference' is unsupported because eigendecomposing the learned mass matrix M(q) at inference is not obviously cheaper than direct inversion. That is a correctness/evidence gap, not a circularity. The only in-group citations—PIP-Loco [19], barrier reward [24], and MDR-MPC [16]—frame the deployment architecture and reward shaping, but the comparative LNN results stand independently of whether those cited works are correct; no load-bearing claim reduces to a self-citation. Overall, the derivation chain is not circular; the score reflects minor self-citation and an unverified speed-up premise, not a constructed equivalence.

Assumptions & free parameters 3 free parameters · 6 assumptions · 1 invented entities

The central empirical comparison does not depend on a hand-fit physical constant. Instead it depends on several modeling assumptions: the Euler-Lagrange structure is the right inductive bias, the learned mass matrix parameterization is expressive enough, Isaac Gym states are treated as ground truth, and a state estimator can recover full state from partial observations. The diagonalization speed-up also carries an unverified computational-cost assumption. Network weights and the regularizer epsilon are fitted or hand-chosen parameters, but they are not physical constants.

free parameters (3)
  • Positive-definiteness regularizer epsilon in mass matrix (Eq 6)
    Introduced by hand to keep M(q) invertible; no value or sensitivity analysis is reported.
  • Learned network weights (LNN, state estimator, Dreamer, force estimator)
    All fitted to Isaac Gym simulator data; predictions depend entirely on these trained weights. No seed or uncertainty reporting is provided.
  • Hidden layer sizes for actor-critic and encoder/Dreamer = [512,256,128] and [256,256]
    Architecture choices chosen without ablation, though they are not fitted to data.
assumptions (6)
  • standard math Euler-Lagrange equations govern the learned dynamics (Eq 8, Eq 12)
    The LNN derives accelerations from L = qdot^T M(q) qdot - V(q); this is the standard mechanical prior.
  • domain assumption The learned mass matrix is positive definite via M = YY^T + epsilon*I (Eq 6)
    Assumes the parameterization is invertible and expressive enough to cover the true inertia matrix; no evaluation of this representational assumption is given.
  • domain assumption Isaac Gym simulator provides ground-truth states for supervised training
    All claims about prediction accuracy are measured against simulated states, not hardware.
  • domain assumption A state estimator E_theta can recover the full 18-dimensional state q from partial observations (Eq 5)
    The LNN operates in full state space while observations are partial; estimator errors are not analyzed.
  • domain assumption The actuator network [23] converts commanded joint angles to torques accurately
    Inverse-dynamics and control-frequency analysis rely on this conversion, but the actuator model is taken from prior work without validation here.
  • standard math Eigen-decomposition of a symmetric matrix yields P and Lambda and is a valid way to compute M^{-1} (Eq 10-11)
    Standard linear algebra, but the computational-cost premise that this reduces complexity is not proven.
invented entities (1)
  • Learned external force estimator F_theta
    purpose: Accounts for external forces in the forward dynamics (Eq 8)
    A neural network residual model fitted to simulator data; no independent falsifiable prediction or physical interpretation is provided.

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Cite this review

Pith. "Pith review of Investigating Lagrangian Neural Networks for Infinite Horizon Planning in Quadrupedal Locomotion." pith.science (2026). https://pith.science/paper/KCUMCG4Q

@misc{pith2026250616079,
  author       = {Pith},
  title        = {Pith review of: Investigating Lagrangian Neural Networks for Infinite Horizon Planning in Quadrupedal Locomotion},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/KCUMCG4Q}},
  note         = {Machine review of arXiv:2506.16079}
}
read the original abstract

Lagrangian Neural Networks (LNNs) present a principled and interpretable framework for learning the system dynamics by utilizing inductive biases. While traditional dynamics models struggle with compounding errors over long horizons, LNNs intrinsically preserve the physical laws governing any system, enabling accurate and stable predictions essential for sustainable locomotion. This work evaluates LNNs for infinite horizon planning in quadrupedal robots through four dynamics models: (1) full-order forward dynamics (FD) training and inference, (2) diagonalized representation of Mass Matrix in full order FD, (3) full-order inverse dynamics (ID) training with FD inference, (4) reduced-order modeling via torso centre-of-mass (CoM) dynamics. Experiments demonstrate that LNNs bring improvements in sample efficiency (10x) and superior prediction accuracy (up to 2-10x) compared to baseline methods. Notably, the diagonalization approach of LNNs reduces computational complexity while retaining some interpretability, enabling real-time receding horizon control. These findings highlight the advantages of LNNs in capturing the underlying structure of system dynamics in quadrupeds, leading to improved performance and efficiency in locomotion planning and control. Additionally, our approach achieves a higher control frequency than previous LNN methods, demonstrating its potential for real-world deployment on quadrupeds.

Figures

Figures reproduced from arXiv: 2506.16079 by the authors.

Figure 1
Figure 1. Traditional neural networks (Simple NN) learn dynamics in a purely [PITH_FULL_IMAGE:figures/full_fig_p001_1.png] view at source ↗
Figure 2
Figure 2. The framework leverages physics-inspired dynamics within a Dreamer-based model to ensure physical consistency in quadruped locomotion. The [PITH_FULL_IMAGE:figures/full_fig_p003_2.png] view at source ↗
Figure 4
Figure 4. Prediction error of different dynamics models compared to actual state [PITH_FULL_IMAGE:figures/full_fig_p005_4.png] view at source ↗
Figures from the paper (2 more)
Figure 3
Figure 3. Figure 3: Dynamics loss graph plotted on a logarithmic scale for better [PITH_FULL_IMAGE:figures/full_fig_p005_3.png]
Figure 5
Figure 5. Figure 5: Controller inference frequency variation of different dynamics models. [PITH_FULL_IMAGE:figures/full_fig_p005_5.png]

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Reference graph

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